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A Tribute to Max Von Laue

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A Tribute to Max Von Laue FEATURES A Tribute to Max von Laue Henk Kubbinga, University of Groningen (The Netherlands) DOI: 10.1051/epn/2012602 20 EPN 43/6 Article available at http://www.europhysicsnews.org or http://dx.doi.org/10.1051/epn/2012602 MAX VON LAUE FEATURES Just an idea: take a crystal, surround it with photographic plates, and direct a pencil of X-rays at it, perpendicularly. It was one of those thrilling ideas that made new science. Max Laue was the proponent, in April 1912. The experiment as such had been tried out before by Röntgen himself, but without avail. Friedrich and Knipping, however, took their time and waited long enough. Overnight, the atomic variant of lattice theory—which had worked its way at the outskirts of crystallography—became fashionable. And, not to forget, X-rays proved to be wave-like indeed. ax Laue originated from Pfaffendorf, Rays and rays and… X-rays b P.18: Blende (ZnS; a village now part of Koblenz. After At the turn of the XIXth and XXth century a whole series covered with calcite) from Trepca (Serbia). his Abitur he enrolled at the university of seemingly distinct, though more or less related radia- Aquarelle by Claus of Strasbourg, moving on, in 1899, to tion phenomena disputed each other's priority in the Caspari (1911-1980). Göttingen, the place to be for theoreticians. Optics physicists' attention. One of the most enigmatic was, Reproduced from M H. Schröcke and became his favourite subject. Waldemar Voigt and without doubt, the one revealed by Wilhelm Röntgen in K.l. Weiner, Otto Lummer showed the way to go. His PhD sub- the fall of 1896. For the general public, however, it had Mineralien (Hamburg: ject brought him to Berlin to study with Max Planck. been overshadowed, by some natural rays, spontane- E. Cramer, 1967). In 1903 Laue defended a thesis about the diffraction ously emitted by materials that could be concentrated which occurs during interference caused by plane by chemical means. Laue got involved in 1909 when he parallel plates. It was Planck who asked him, in 1906, entered, as a Privatdozent, in the service of Arnold Som- to become his assistant. Laue's Habilitation assessed merfeld, at the University of Munich. Sommerfeld him- the entropy of interfering pencils of rays. It was the self had been nominated a few years before to provide time that one Albert Einstein's freshly appeared paper the theoretical background to Röntgen's rays. Röntgen 'Zur Elektrodynamik bewegter Körper' was favorably was still around, but left Sommerfeld and the latter's stu- discussed by Planck in a lecture at the Colloquium of dents free to use his instruments, among which a 50 cm Berlin's Physical Society. Rühmkorff-inductor and a whole collection of bulbs. Relativity: theory and experiment Lattice theory in crystallography Laue was in the audience. It took some time, but his con- The 19th century had lived with the rise of lattice theo- version was unconditional. He went to see Einstein in ry. Crystals had been conceived of, by René-Juste Haüy Switzerland, soon after his Habilitation, to discuss details. (1743-1822), as well-ordered 'assemblages' of polyhedral His was one of the first experimental arguments if not proofs (1907), in the sense that he identified Einstein's 'ad- dition theorem' with a formula derived by Fizeau (1851) for the velocity of light in flowing water. Fizeau, it is re- called, first established (together with Foucault) that in denser media light is slowed down—in conformity with the wave-theory—while the motion of some such medium may be used to move an interference pattern: the fringes produced by coherent light led through the two arms of a water circuitry slightly shifted when the flow direction was changed. Fizeau did not insist and left others the task to improve his method. It was Michelson and Morley who did so in 1887. There were some problems with the turbu- lence of the flowing water and Pieter Zeeman, therefore, used a movable glass stick instead. Laue produced the first general account of the recent developments in Das Rela- tivitätsprinzip (1911) and succeeded in familiarizing many an estranged physicist with the broad context—and the paradoxes—of what came to be known as special relativ- b FIG. 1: Max von ity. In 1920 he would publish, as a supplement, a similar Laue (1920; courtesy account of Einstein's latest breakthrough, general relativity. Nobel Foundation). EPN 43/6 21 FEATURES MAX VON LAUE molecules composed of the atoms of the elements. Those of the exact number of a priori possible atomic lattices (230) pyrite, for instance, were presented as 'assemblages' of cubic was rigorously deduced by mathematicians like Evgrad FeS2-molecules. Such 'assemblages' could take the form of Fyodorov and Arthur Schönflies. When Laue arrived in a cube or orthogonal parallellepiped, naturally, but also Munich Sohncke's spirit was still in the air, while the lat- that of a dodecahedron or octahedron, depending on the ter's lattice models had survived and were regularly used regularities during the growth. It was a personal triumph in classes. There was a third lucky coincidence. for Haüy not only that the interfacial angles could be cal- culated in advance, but also that they agreed closely with Encyclopedia of the mathematical sciences those measured on natural crystals, for instance, in the case Felix Klein and Sommerfeld had launched, in 1896, the of dodecahedral pyrite. His successors gradually replaced great Encyclopedia of the mathematical sciences, which the molecules by their centres of gravity. In this way the became the indispensable toolkit for any physicist, let's crystal became an abstract point lattice whose symmetry say, together with the ever growing Physikalisch-Chemis- properties defied the imagination of men like Delafosse, che Tabellen of Landolt and Börnstein. Once established Bravais and Jordan. Particular compounds, like the alums, in Munich, Laue was chartered to assess the theory and though, suggested the existence of superimposed molecular practice of wave-optics and had, naturally, amongst many lattices: after all, the crystal water of these so-called hydrates other things, to assess interference phenomena [1]. That could be easily separated from the rest, while a crystal of wave-optics was part of volume V of the Encyclopedia…, the original form emerged on evaporating a solution. It which for all kind of reasons—i.a. the Great War—would was Leonhard Sohncke (1842-1897) who concluded, in not appear in print before the 1920's. The text, it is true, 1888, that any crystal could be considered as an array of as only assessed line gratings, but during its preparation many lattices as there are atomic species in it. In the 1890's Laue had become familiar with experiments with crossed gratings, when square arrays of identical spots show up, . FIG. 2: The original set-up as used by Friedrich and Knipping to see the effect of X-rays on a copper square spots, that is. The stage was set. sulfate crystal. From left to right on the table: Röntgen bulb (too low here), first diaphragm (lead foil), collimator, round turntable with the crystal at its centre and an enveloped photographic plate. A huge wooden tripod is used to rise and reset a shielding cover of lead foil. Since 1921 this set-up is part of the Crystals and X-rays collection of the Deutsches Museum, München (courtesy: Deutsches Museum). Having finished his Encyclopedia… contribution, it oc- curred to Laue, early in 1912, that something interesting might happen when a pencil of X-rays would be directed at a crystal, the more so since the estimated wavelength of Röntgen's rays (on spectral grounds: 10-8-10-9 cm) was equal if not smaller than the interatomic distance (10-8 cm). An exchange of ideas, in February 1912, with Paul Ewald triggered a wider discussion at the Institute. An experiment, then, was staged, by Walther Friedrich and Paul Knipping. In a search for effects an easily grown copper sulphate crys- tal (triclinic) was first bombarded with X-rays, with pho- tographic plates at various positions around it (Figure 2). They found that a plate behind the crystal manifested distinct black spots suggesting some kind of regularity. It was a small step, then, to replace the raw crystallized copper sulphate crystal by a thin 001 platelet of highly symmetric zinc sulfide (thickness: 0.5 mm; Figure 3). The result was a breathtakingly regular pattern of spots, manifesting the same symmetry elements as those deduced earlier for the crystal itself (Figure 4): a fourfold main ro- tation axis and four twofold rotation axes (four planes of symmetry). On enlarging the distance between the crystal and the photographic plate (say, P5 instead of P4), the spots kept their bigness and form, though the scale of the pattern was enlarged in the same proportion: apparently a parallel beam of rays was responsible for each spot. In the publica- tion Laue would show how the distance between the cen- tres of gravity of two neighbouring ZnS-molecules could be calculated, using the density ρ = 4.06 g.cm-3, the molar 23 weight M = 97.4 g and Avogadro's constant, NA = 6.17×10 : 22 EPN 43/6 MAX VON LAUE FEATURES [97.4/{4.06×(6.17×1023)}]⅓ = 3.38×10-8 cm. This would be the lattice constant. It brought Laue, Friedrich and Knipping instantaneous fame. In 1913 and, again, in 1914, Laue was nominated for the Nobel Prize for Physics. There were but few nominations, it is true, but these were enough for the Selection Committee to decide in 1914 in favor of Laue.
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